On the horseshoe drag of a low-mass planet. II Migration in adiabatic disks

TL;DR

This paper analyzes the horseshoe drag on a low-mass planet in adiabatic disks, revealing an additional entropy-related torque component and its dependence on disk parameters, which influences planetary migration.

Contribution

It introduces a new torque term related to entropy gradients in adiabatic disks, extending classical horseshoe drag theory and highlighting effects in three-dimensional scenarios.

Findings

Additional torque term scales with entropy gradient

Evanescent waves at horseshoe separatrices influence torque

Torque strength depends steeply on potential softening length

Abstract

We evaluate the horseshoe drag exerted on a low-mass planet embedded in a gaseous disk, assuming the disk's flow in the coorbital region to be adiabatic. We restrict this analysis to the case of a planet on a circular orbit, and we assume a steady flow in the corotating frame. We also assume that the corotational flow upstream of the U-turns is unperturbed, so that we discard saturation effects. In addition to the classical expression for the horseshoe drag in barotropic disks, which features the vortensity gradient across corotation, we find an additional term which scales with the entropy gradient, and whose amplitude depends on the perturbed pressure at the stagnation point of the horseshoe separatrices. This additional torque is exerted by evanescent waves launched at the horseshoe separatrices, as a consequence of an asymmetry of the horseshoe region. It has a steep dependence on the potential's softening length, suggesting that the effect can be extremely strong in the three dimensional case. We describe the main properties of the coorbital region (the production of vortensity during the U-turns, the appearance of vorticity sheets at the downstream separatrices, and the pressure response), and we give torque expressions suitable to this regime of migration. Side results include a weak, negative feed back on migration, due to the dependence of the location of the stagnation point on the migration rate, and a mild enhancement of the vortensity related torque at large entropy gradient.